Abstract

Operators satisfying Clifford algebra (fermions) and Weyl algebra (bosons) are introduced. F(4) and G(3) are realized in terms of bilinears of fermions (the even part) and bilinears of one boson and one fermion (the odd part). D(2,1;α) is realized as bilinears (the even part) and trilinears (the odd part) of bosons.